{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.82127.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1609848"}}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"A search is presented for single production of heavy vector-like quarks (B) that decay to a Higgs boson and a b quark, with the Higgs boson decaying to a highly boosted bb pair reconstructed as a single collimated jet. The analysis is based on data collected by the CMS experiment in proton-proton collisions at \u221as = 13 TeV, corresponding to an integrated luminosity of 35.9fb\u22121. The data are consistent with background ex- pectations, and upper limits at 95% confidence level on the product of the B quark cross section and the branching fraction are obtained in the range 1.28\u20130.07 pb, for a narrow B quark with a mass between 700 and 1800 GeV. The production of B quarks with widths of 10, 20 and 30% of the resonance mass is also considered, and the sen- sitivities obtained are similar to those achieved in the narrow width case. This is the first search at the CERN LHC for the single production of a B quark through its fully hadronic decay channel, and the first study considering finite resonance widths of the B quark.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t1","@type":"Dataset","description":"Distribution in the reconstructed B quark mass after applying all selections to events with no forward jets and in the...","name":"Table1"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t2","@type":"Dataset","description":"Distribution in the reconstructed B quark mass after applying all selections to events with at least one forward jet and...","name":"Table2"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t3","@type":"Dataset","description":"Distribution in the reconstructed B quark mass after applying all selections to events with no forward jets and in the...","name":"Table3"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t4","@type":"Dataset","description":"Distribution in the reconstructed B quark mass after applying all selections to events with no forward jets and in the...","name":"Table4"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t5","@type":"Dataset","description":"Distribution in the reconstructed B quark mass after applying all selections to events with no forward jets and in the...","name":"Table5"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t6","@type":"Dataset","description":"Distribution in the reconstructed B quark mass after applying all selections to events with at least one forward jet and...","name":"Table6"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t7","@type":"Dataset","description":"Distribution in the reconstructed B quark mass after applying all selections to events with no forward jets and in the...","name":"Table7"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t8","@type":"Dataset","description":"Distribution in the reconstructed B quark mass after applying all selections to events with at least one forward jet and...","name":"Table8"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t9","@type":"Dataset","description":"The median observed and expected 95% CL upper limits on the product of the B quark production cross section and...","name":"Table9"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t10","@type":"Dataset","description":"The median observed and expected 95% CL upper limits on the product of the B quark production cross section and...","name":"Table10"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t11","@type":"Dataset","description":"The median observed and expected 95% CL upper limits on the product of the B quark production cross section and...","name":"Table11"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t12","@type":"Dataset","description":"The median observed and expected 95% CL upper limits on the product of the B quark production cross section and...","name":"Table12"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t13","@type":"Dataset","description":"Observed and expected fitted number of events in the signal ranges of 800 < mB < 1500, and expected signal...","name":"Table13"},{"@id":"https://doi.org/10.17182/hepdata.82127.v1/t14","@type":"Dataset","description":"Observed and expected fitted number of events in the signal ranges 1500 < mB < 1800 , and expected signal...","name":"Table14"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1609848?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/82127"}],"inLanguage":"en","name":"Search for a singly produced vector-like quark B decaying to a b quark and a Higgs boson in a fully hadronic final state using boosted topologies","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1609848?version=1","version":1}